Diffractive grating coupled whispering gallery mode resonators

ABSTRACT

Optical resonators and optical devices based on optical resonators that implement diffractive couplers for coupling light with the optical resonators.

PRIORITY CLAIM AND RELATED APPLICATION

This application claims the benefit of U.S. Provisional Application No. 60/934,799 entitled “Diffractive Coupler for High-Q Whispering-Gallery Microresonators” and filed Jun. 13, 2007, the disclosure of which is incorporated by reference as part of the specification of this application.

BACKGROUND

This application relates to optical resonators and optical devices based on optical resonators.

Optical resonators may be used to spatially confine resonant optical energy in a limited cavity with a low optical loss. The resonance of an optical resonator may be used to provide various useful functions such as optical filtering, optical modulation, optical amplification, optical delay, and others. Light can be coupled into or out of optical resonators via various coupling mechanisms according to the configurations of the resonators. For example, Fabry-Perot optical resonators with two reflectors at two terminals may use partial optical transmission of at least one reflector to receive or export light.

Optical whispering gallery mode (WGM) resonators confine light in a whispering gallery mode that is totally reflected within a closed circular optical path. Unlike Fabry-Perot resonators, light in WGM resonators cannot exit the resonators by optical transmission. Light in a WGM resonator “leaks” out of the exterior surface of the closed circular optical path of a WGM resonator via the evanescence field of the WG mode. An optical coupler can be used to couple light into or out of the WGM resonator via this evanescent field.

SUMMARY

The specification of this application describes, among others, examples and implementations of diffractive grating couplers for WGM resonators.

In one example, an optical device, includes: an optical resonator structured to support a whispering gallery mode circulating in a plane of the optical resonator; and a diffractive grating coupler comprising a substrate and a phase-type diffractive grating formed in the substrate, the diffractive grating coupler being located close to the optical resonator to evanescently couple an input optical beam incident at a normal incidence to one side of the substrate of the diffractive grating into the optical resonator located on the other side of the substrate of the diffractive grating. The diffractive grating is structured to suppress diffracted light along the normal incidence and diffract light of the input optical beam into a first diffraction order at a first side of the normal incidence that matches in phase with light in the whispering gallery mode along a first circulating direction and a second diffraction order at a second side of the normal incidence that matches in phase with light in the whispering gallery mode along a second circulating direction opposite to the first circulating direction to create a standing wave in the whispering gallery mode inside the optical resonator.

In another example, an optical device includes an optical resonator structured to support a whispering gallery mode circulating in a plane of the optical resonator; and a diffractive grating coupler located adjacent to and optically coupled to the optical resonator. This diffractive grating coupler includes a fiber comprising a fiber core and a fiber cladding surrounding the fiber core, wherein the fiber core comprises a fiber grating section configured to diffract guided light in the fiber core into the fiber cladding toward the an end facet of the fiber, and wherein the fiber is located to place the end facet adjacent to a surface of the optical resonator to provide optical coupling with the optical resonator; and a phase-type diffractive grating formed on the end facet to evanescently couple light between the fiber and the optical resonator, wherein the diffractive grating is structured to suppress diffracted light in a zero diffraction order and diffract light of the input optical beam into light in at least one of two first diffraction orders that matches in phase with the whispering gallery mode inside the optical resonator.

These and other examples and implementations are described in detail in the drawings, the detailed description, and the claims.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 shows an example of an optical device where a WGM resonator is coupled to two diffractive phase grating couplers in the normal incidence configuration to provide optical input and output.

FIG. 2 shows an example of a diffractive grating coupler for use in FIG. 1.

FIG. 3 shows one example of operation of a fiber grating coupler for a WGM resonator.

FIGS. 4, 5 and 6 show examples of different operations of fiber grating couplers for WGM resonators.

FIGS. 7 and 8 show two different fiber grating couplers for WGM resonators.

FIGS. 9 and 10 show operations of the two fiber grating couplers in FIGS. 7 and 8, respectively.

DETAILED DESCRIPTION

The grating couplers described in this application can be used in various configurations. In one configuration, for example, such grating couplers can be used to implement a normal-incidence coupling method for microresonators. Normally incident beam, or propagating mode of a waveguide is shaped to match the evanescent field envelope during contact of coupler with a spheroidal microresonator by means of, for example, a GRIN lens, or a mode expander in waveguide structure. A phase-type diffratice grating is fabricated at the interface surface of the normal-incidence coupler. This grating couples the incident beam simultaneously to clockwise and counter-clockwise traveling WG modes in the microresonator (upon normal incidence), minus first and plus first diffractive orders. Hence, the incident beam effectively excites a standing WG mode. With angled excitation, the optimal phase grating can excite exclusively minus first order of diffraction and therefore be capable of coupling into uni-directional (traveling wave) whispering-gallery mode.

Under the normal incidence configuration for generating a standing-wave excitation in the resonator, the coupling is optically reciprocal and therefore the resonator provides optical feedback into the coupler. As such, the optical feedback can be used to inject into a laser. This feedback, which is resonant at the frequency of WG mode, can be used for injection locking the low-Q laser such as semiconductor diode Fabry-Perot (FP), or distributed feedback (DFB) laser to suppress frequency fluctuations and narrow the laser linewidth.

FIG. 1 shows an example of an optical device where a WGM resonator is coupled to two diffractive phase grating couplers in the normal incidence configuration to provide optical input and output. This device includes an optical resonator structured to support a whispering gallery mode circulating in a plane of the optical resonator and a first diffractive grating coupler that is coupled to the optical resonator to send light into the optical resonator as an input port on the top of the resonator. A second diffractive phase grating coupler is provided at a different location to couple light out of the optical resonator as an optical output port. The optical output of this output port may be directed into an optical detector as shown or other device. Each grating coupler is paired with a lens assembly for shaping the light to or from the grating coupler. Such a lens assembly can include multiple lens elements such as two different GRIN lens segments with different numerical apertures.

In one implementation, such a diffractive grating coupler can include a substrate and a phase-type diffractive grating formed in the substrate. The diffractive grating coupler is located close to the optical resonator to evanescently couple an input optical beam incident at a normal incidence to one side of the substrate of the diffractive grating into the optical resonator located on the other side of the substrate of the diffractive grating. The diffractive grating structured to suppress diffracted light along the normal incidence and diffract light of the input optical beam into a first diffraction order at a first side of the normal incidence that matches in phase with light in the whispering gallery mode along a first circulating direction and a second diffraction order at a second side of the normal incidence that matches in phase with light in the whispering gallery mode along a second circulating direction opposite to the first circulating direction to create a standing wave in the whispering gallery mode inside the optical resonator.

In FIG. 1, a laser can be located near the lens assembly as the optical beam shaping device to direct a laser beam as the optical input beam into the optical beam shaping device and to receive feedback light from the optical beam shaping device and the diffractive grating coupler that is received by the diffractive grating via evanescent light of light in the whispering gallery mode at the surface of the optical resonator. Under this configuration, the laser is locked to an optical frequency of the received feedback light due to optical injection locking.

FIG. 2 shows an example of a diffractive grating coupler for use in FIG. 1. A grating substrate is provided to support an optical phase grating on the substrate. The grating substrate can be an end facet of a fiber or a surface of other optical devices.

An optical fiber can be configured to include a fiber grating as a grating coupler for WGM resonators to provide grating assisted coupling.

FIG. 3 shows one example of operation of a fiber grating coupler for a WGM resonator where the wave vector space diagram is also shown. Such a fiber'grating is usually used to do phase matching between modes of the coupler and the WGM resonator. In multimode cavities grating couples mode of the coupler (dashed line on left diagram) into many modes of the resonator (three solid red lines). Evanescent field of deeper modes in whispering gallery resonators weakly depend on mode depth. This results in low coupling into +1 diffraction order mode. The zero diffraction order can be suppressed by using of very efficient grating, but side orders tend to have equal efficiencies.

FIGS. 4, 5 and 6 show examples of different operations of fiber grating couplers for WGM resonators.

FIG. 4 shows grating assisted coupling for a standing wave coupling into the WGM resonator. A short period phase grating with large Kgrating value can be used to achieve this operation where the Zero order is suppressed and the plus and minus first diffraction orders correspond to exactly the same whispering gallery mode.

FIG. 5 shows grating assisted coupling for a traveling wave coupling into the WGM resonator. This example uses even shorter period phase grating with large Kgrating value. The zero order is suppressed and the minus first diffraction order is suppressed since phase matching conditions for this kind of mode are not satisfied. Coupling is efficient only to one traveling mode.

FIG. 6 shows the bandwidth of grating assisted coupling bandwidth of the coupling. Grating with unlimited length couples only one mode to only one mode. A phase grating with period A and limited length L couples many modes to many modes. In order to increase selectivity of the coupler the length of the grating is be increased.

FIG. 7 shows a fiber diffractive grating coupler that can be located adjacent to and optically coupled to an optical WGM resonator. This diffractive grating coupler includes a fiber that includes a fiber core and a fiber cladding surrounding the fiber core. The fiber core includes a fiber grating section configured to diffract guided light in the fiber core into the fiber cladding toward the an end facet of the fiber, and the fiber is located to place the end facet adjacent to a surface of the optical resonator to provide optical coupling with the optical resonator. A phase-type diffractive grating is formed on the end facet to evanescently couple light between the fiber and the optical resonator. The diffractive grating is structured to suppress diffracted light in a zero diffraction order and diffract light of the input optical beam into light in at least one of two first diffraction orders that matches in phase with the whispering gallery mode inside the optical resonator.

In one configuration, the fiber is oriented to be perpendicular to the surface of the optical resonator to diffract input light into the two first diffraction orders that match in phase with two light waves in the whispering gallery mode inside the optical resonator that propagate in opposite directions to form a standing wave inside the optical resonator.

In another configuration, the fiber is oriented to form an angle with respect to a normal direction of the surface of the optical resonator to diffract input light into only one first diffraction order that matches in phase with the whispering gallery mode inside the optical resonator to generate a uni-directional traveling wave inside the optical resonator.

FIG. 8 shows a fiber grating coupler with the grating section in the core. This design leads to a small aperture optical phase grating on the fiber end facet and can be used in certain devices. FIGS. 9 and 10 show operations of the two fiber grating couplers in FIGS. 7 and 8, respectively

While this specification contains many specifics, these should not be construed as limitations on the scope of an invention or of what may be claimed, but rather as descriptions of features specific to particular embodiments of the invention. Certain features that are described in this specification in the context of separate embodiments can also be implemented in combination in a single embodiment. Conversely, various features that are described in the context of a single embodiment can also be implemented in multiple embodiments separately or in any suitable subcombination. Moreover, although features may be described above as acting in certain combinations and even initially claimed as such, one or more features from a claimed combination can in some cases be excised from the combination, and the claimed combination may be directed to a subcombination or a variation of a subcombination.

Only a few implementations are disclosed. However, it is understood that variations, enhancements and other implementations can be made based on what is described and illustrated in this patent application. 

1. An optical device, comprising: an optical resonator structured to support a whispering gallery mode circulating in a plane of the optical resonator; and a diffractive grating coupler located adjacent to and optically coupled to the optical resonator, the diffractive grating coupler comprising: a fiber comprising a fiber core and a fiber cladding surrounding the fiber core, wherein the fiber core comprises a fiber grating section configured to diffract guided light in the fiber core into the fiber cladding toward the an end facet of the fiber, and wherein the fiber is located to place the end facet adjacent to a surface of the optical resonator to provide optical coupling with the optical resonator; and a phase-type diffractive grating formed on the end facet to evanescently couple light between the fiber and the optical resonator, wherein the diffractive grating is structured to suppress diffracted light in a zero diffraction order and diffract light of the input optical beam into light in at least one of two first diffraction orders that matches in phase with the whispering gallery mode inside the optical resonator.
 2. The device as in claim 1, wherein: the fiber is oriented to be perpendicular to the surface of the optical resonator to diffract input light into the two first diffraction orders that match in phase with two light waves in the whispering gallery mode inside the optical resonator that propagate in opposite directions to form a standing wave inside the optical resonator.
 3. The device as in claim 1, wherein: the fiber is oriented to form an angle with respect to a normal direction of the surface of the optical resonator to diffract input light into only one first diffraction order that matches in phase with the whispering gallery mode inside the optical resonator to generate a uni-directional traveling wave inside the optical resonator.
 4. The device as in claim 1, wherein: the optical resonator is a spheroidal resonator.
 5. The device as in claim 1, comprising: a laser located to direct a laser beam as input light into the fiber of the diffractive grating coupler which couples the input light into the optical resonator via the phase-type diffractive grating formed on the end facet of the fiber and couples light out of the optical resonator as feedback light to the laser, wherein the laser receives the feedback light and is locked to an optical frequency of the received feedback light.
 6. The device as in claim 5, wherein: the laser responds to an input RF signal to modulate the laser beam to carry the input RF signal, the device includes an output optical coupler located close to the optical resonator at a location different from the diffractive grating coupler and operable to evanescently couple light out of the optical resonator to produce an output optical beam; and an optical detector that receives the output optical beam from the output optical coupler to convert the received output optical beam into an RF signal indicative of the input RF signal.
 7. The device as in claim 1, wherein: the phase-type diffractive grating formed on the end facet is structured to have a dimension similar to a cross section of the fiber core.
 8. The device as in claim 1, wherein: the phase-type diffractive grating formed on the end facet is structured to have a dimension greater than a cross section of the fiber core. 